Apparatus for noninvasive measurement of properties of a fluid flowing in a tubing having a smaller inner diameter passage

ABSTRACT

Apparatus for non-invasive measuring of the sound velocity of a fluid flowing in a tubing having a small internal diameter for the fluid passage as compared to the tubing wall thickness and having points of two different and known transverse length with a sensor mounted at each point and a delay line adjacent to the tubing at each point. Each sensor is connected to a circuit that provides ultrasonic energy signals that are transmitted through the tubing walls, the flowing fluid and the delay line to be reflected back to the sensor from which the round trip transit time of the signals is measured and the sound velocity calculated from the two measured round trip transit times and the differential between the known transverse lengths.

RELATED APPLICATION

This application is a continuation-in-part of application Ser. No. 12/959,496, filed Dec. 3, 2010 by the same inventor of the subject application and entitled APPARATUS AND METHOD FOR NON-INVASIVE MEASUREMENT OF PROPERTIES OF A FLUID FLOWING IN A FLEXIBLE TUBING OR CONDUIT

FIELD OF THE INVENTION

The present invention relates to an apparatus and method for non-invasively measuring the sound velocity of a fluid flowing in flexible or rigid tubing and particularly one having a small internal diameter passage in which the fluid flows.

BACKGROUND OF THE INVENTION

The term “sound velocity” is a recognized shorthand expression describing a characteristic of the speed at which sound waves travel in a medium. The speed of sound varies depending on the medium through which the sound waves pass. It usually is a parameter used in describing properties of different substances or mediums. Knowing the value of the sound velocity of a particular medium, such as a flowing fluid, liquid or gas, permits many different characteristics or properties of the fluid to be determined. Using the sound velocity together with appropriate mathematical relationships allows for determination of various characteristics or properties of the medium such as its density, purity concentration, components of the medium composition, etc.

Several different types of apparatus exist for measuring the velocity of a signal, hereafter referred to as the “sound velocity”, in a fluid flowing in flexible or rigid conduit type tubing. The term “tubing” is used hereafter to define both the flexible and rigid type except as otherwise expressly disclosed. The different apparatus types for measuring sound velocity generally are of either the contact or the non-invasive type. In the contact type, some part or parts of the measuring apparatus come into direct contact with the fluid. In the non-invasive type, the sound velocity is measured without any part of the measuring apparatus coming into contact with the fluid.

In many applications it is preferred that the sound velocity measurement be made non-invasively. The non-invasive measurement has advantages in medical and biotechnology applications, as well as in handling hazardous chemicals and ultra pure liquids such as are used in semiconductor processing systems. The advantages primarily result from the fact that no part of the measuring apparatus comes in contact with the fluid that might lead to contamination while making the measurements needed to determine the sound velocity. Also, when dealing with hazardous and corrosive fluids possible damage to parts of the measuring apparatus is avoided since there is no contact with the fluid.

Several instruments are known for making the sound velocity measurement non-invasively. For example, in U.S. pre-grant patent publication 2006/0052963 two pairs of ultrasonic transducers, or sensors, are used. One of the sensors of each pair is a transmitter of ultrasonic (electro-mechanical) signal energy and the other is a receiver. The transmitting and receiving sensors of each pair are mounted on opposite sides of the tubing in which the fluid is flowing. The transit time of a signal from the transmitting sensor of each pair along a respective path through the fluid and the two tubing walls to the receiving sensor of the pair is measured. The sound velocity of the signal in the liquid is calculated from the results of the two one-way transit time measurements. While such apparatus is effective in determining the sound velocity, it requires four sensors. Also, in some of the disclosed embodiments a special mounting is required for the sensors of the two pairs so that the transmitter and receiver sensors are offset at an angle from the tubing wall and from each other along the tubing length. Here the ultrasonic signal is transmitted by one sensor of each pair upstream and downstream of the fluid flow to the other sensor of the pair on the tubing opposite side.

In U.S. Pat. No. 7,481,114 a flexible tubing is mounted in a fixture having a device that produces a force to deform the tubing external and internal dimensions at one point in a direction transverse to the tubing length. The tubing cross-sectional dimensions are hereafter referred to as “transverse length” since they are in a direction that is perpendicular to the tubing longitudinal axis and the fluid flowing in it. The force producing device deforms the normally circular flexible tubing cross section by a first amount to form a first path, or transverse length. The first path has a first acoustic path length along which a signal is transmitted by an ultrasonic sensor and reflected back to the sensor after reflection from the opposing internal wall of the deformed tubing. The round trip signal transit time along the first path is measured. The force producing device is operated again to further deform the tubing transverse length dimension to form a second path which is co-linear with the first path but that has an acoustic path length different from that of the first path. A signal is transmitted by the sensor and reflected back to it along the second co-linear path. The round trip transit time of the signal along the second path is measured. The sound velocity is then calculated based on the two measured round trip transit times. In this system the separate force producing device must be provided and some apparatus also must be provided for operating this device at the proper times in relation to the transmission and reception of the signals over the two paths. This effectively prevents sound velocity from being measured on a substantially continuous basis. Also, the apparatus cannot work with rigid tubing.

Accordingly, it is desired to provide a more simplified apparatus and method for accomplishing non-invasive measurement of the sound velocity of a flowing fluid in a tubing which can be done on a continuous basis and particularly an apparatus and method that accurately functions with tubing having a small internal diameter passageway through which the fluid flows.

BRIEF DESCRIPTION OF THE INVENTION

In accordance with the invention, as described in the aforesaid application, an apparatus is provided to non-invasively measure sound velocity in a fluid flowing in either elastic or rigid tubing. Elastic tubing is made of an elastomeric material that can be deformed or squeezed to change its cross-sectional, or transverse, length. In the invention, a single sensor is mounted at two different points of the tubing that have different transverse lengths. A pulse echo technique is used to measure the round-trip transit time of a signal that is transmitted by the sensor at each of the two tubing points along an acoustic path through a wall of the tubing and reflected back to the sensor from the tubing opposing internal wall. The round trip transit time of the signal for each of the two paths is measured. The transit times are different because of the different transverse lengths of the tubing and the acoustic paths at each of the two points where the measurements take place. By knowing the differential between the transverse lengths of the tubing at the two points and the results of the two round-trip transit time measurements the sound velocity of the fluid flowing in the tubing can be calculated. The sound velocity calculation is independent of the tubing wall thickness.

In one embodiment of the invention for use with elastic tubing, the tubing is held in the elongated slot of a measuring head in which the slot has two sections of different known transverse lengths (distances across the slot). When placed in the slot, the elastic tubing is deformed, or squeezed, into a somewhat elliptical shape and the tubing is firmly held in the slot. One sensor is placed in the measuring head adjacent to the tubing at a point of each slot section. Each sensor both transmits signal energy though the wall of the tubing to be reflected from the opposing inner wall back to the sensor. The measured value of the round-trip transit time of the signal energy transmitted along a path to and reflected from the tubing internal wall at each point will be different because of the different outer transverse lengths of the deformed tubing at the two points along the tubing length. The differential of the transverse lengths at the points of the two sections is known from the construction of the slot or from measurement and the sound velocity is calculated from this and the measured values of the two round trip transit times.

In another embodiment of the invention for use with elastic tubing, there is a measuring head with a slot having one location along its length in which the elastic tubing is placed where it is deformed from its normal circular shape to a more generally elliptical shape. Two sensors are mounted at different points of the single location at an angle, preferably substantially orthogonal, to each other around the tubing. Here, the measured round-trip transit time of the signal from each sensor reflected from the opposing internal tubing wall is different because of the different transverse lengths of the deformed, or squeezed, tubing at the single location. Here also, the sound velocity is calculated using the two measured round-trip transit times and the known differential of the two transverse lengths.

In an embodiment of the invention for measuring the sound velocity of a fluid flowing in rigid tubing, the tubing itself is formed with two, preferably adjacent, sections of different transverse length. The rigid tubing is placed in the slot of a measuring head in which a sensor is mounted at a point of the slot for each tubing section. The round-trip transit time of signals transmitted from each sensor and reflected back to it from the opposing internal wall of the rigid tubing along a respective path is measured. As in the other embodiments, the signal sound velocity is calculated from the two measured round-trip transit times and the known differential of the transverse lengths of the rigid tubing at the two points where the sensors are mounted. Is this embodiment, instead of using a measuring head with a slot, the two sensors can be mounted directly to the wall of the rigid tubing at the two points.

In the various embodiments of the invention a problem can sometimes occur when the internal diameter of the tubing though which the fluid flows is small. For example, certain applications have rigid/flexible tubing as small as 0.5 mm outer diameter and an inner diameter passage through which the fluid flows of less than 0.1 mm. Also, some applications utilize tubing having an outside diameter ten or more times larger than the inner diameter through which the fluid flows. In such types of applications an ultrasonic sensor operating in the pulse echo mode will have multiple reverberation of the transmitted ultrasonic signal and the received ultrasonic signal reflected from the tubing inner wall will be very close in time to these reverberations. Therefore, it becomes difficult to recognize the received signal signature to accurately calculate the round-trip transit time.

To overcome the this problem the invention adds a delay line of a fixed length at the location where the transmitted ultrasonic energy signal is reflected back to the sensor. The delay line is a piece of material in which the ultrasonic signal transmitted from the sensor travels and is reflected back to the sensor from the end of the delay line. The delay line can be of the same or a different material than that of the tubing. In a preferred embodiment of the invention the delay line is of a material in which the ultrasonic signal travels at a slower speed than in the material of the tubing though which the fluid whose sound velocity is being measured flows. The use of the delay line increases the round-trip travel time of the ultrasonic signal and thereby provides a larger time difference between the sensor reverberations and signal reflected back to the sensor which makes it easier to identify the signal. To further improve the accuracy of the measurement, in a preferred embodiment of the invention the electronic circuit that receives the reflected ultrasonic signal to be used in calculating the round-trip transit time is gated open to receive such signal at a time later than the reverberations are produced.

In the various embodiments of the invention that use the two sensors spaced apart, a delay line that provides the same travel time for the ultrasonic signal is provided at each location. In the computation of the fluid sound velocity, the presence of the delay lines at the two locations cancels out so that the accuracy of the computation is not affected.

The delay line can be integral with the tubing, such as a protuberance on its outer wall, or it can be provided as a part of the measuring head. There also can be a reflector of the ultrasonic energy at the end of the delay line most remote from the sensor that transmits and receives the reflected ultrasonic energy.

The use of the delay line with or without a reflector provides for a less cluttered arrival time in which the reflected signal can be more easily identified. This provides for a better and more accurate sound velocity measurement where the invention is used for this purpose.

Each embodiment of the invention includes a microprocessor that controls the times of transmission and reception of the signals by the sensors. The microprocessor is pre-programmed with the known differential value of the transverse lengths at the two points where the sensors are located. The microprocessor also performs the measurements of the two round trip transit times and the calculation of the sound velocity.

In all of embodiments of the invention, only two sensors are required. The transit time measurement for both sensors preferably is made at substantially the same time to minimize the effects of temperature change of the flowing fluid. In all of the embodiments of the invention, the calculation of the sound velocity is independent of tubing wall thickness and change in tubing wall thickness due to temperature changes and tubing material. By eliminating the effect of these external parameters, a more accurate measurement of the sound velocity can be obtained. In using the delay line the calculation of round trip transit time for each sensor also is independent of the delay introduced. Thus, the calculation of the sound velocity is not affected. In the preferred versions all of the embodiments of the invention, the signals are transmitted from and reflected back to each sensor substantially transverse to the tubing longitudinal axis and the fluid flow.

BRIEF DESCRIPTION OF THE DRAWINGS

Other objects and advantages of the present invention will become more apparent upon reference to the following specification and annexed drawings in which:

FIG. 1 is a plan view of a piece of tubing having two sections of different transverse (cross-sectional) length;

FIGS. 1A and 1B are end views of the tubing piece of FIG. 1;

FIG. 2 is a top plan view of an embodiment using a pulse echo technique for measuring the round-trip transit time of signal energy through the tubing at two different points spaced along the length of the slot of a measuring head;

FIG. 3 is an end view in cross-section of a measuring head of an embodiment of the invention in which the two round-trip transit time measurements are made at a single location along the tubing length; and

FIG. 4 is a top view of an embodiment of the measuring head of the invention for making the sound velocity measurement in rigid tubing.

DETAILED DESCRIPTION OF THE INVENTION

Referring to FIGS. 1, 1A and 1B a piece of tubing 10 in which a fluid is flowing is illustratively shown having two sections 10A and 10B of different transverse length. The tubing can be of any material compatible with the fluid to be flowing in it and can transmit ultrasonic (electro-mechanical) energy signals through its wall. The tubing can be of metal or rigid, semi-rigid or deformable plastic. Suitable types of elastomeric deformable plastic are, for example, silicon, Teflon, PVC.

The tubing 10 can have a normal circular cross-section along its length or it can be of other shapes, such as rectangular or square. It is assumed for purposes of explanation, that the tubing 10 of FIG. 1 is part of a longer piece (not shown) of an original shape that has been deformed, or “squeezed”, to be somewhat elliptical along the lengths of the two sections 10A and 10B, as shown by the end views of FIGS. 1A and 1B. The deformation or squeezing takes place for example when elastic tubing 10 is placed in a slot of a measuring head in which the slot transverse length is less than the normal circular, or square or rectangular, elastic tubing outer diameter. Rigid or semi-rigid tubing is pre-formed or supplied with the desired shaped sections 10A and 10B along its length.

As shown in FIGS. 1A and 1B, each section has an extension 11 at a point along its outer wall that provides a delay line function. In a preferred embodiment of the invention the extension 11 delay line is of a material in which ultrasonic signal energy travels at a slower speed than the speed at which travels in walls of the tubing itself. For example, the material of the tubing can be of polyvinylchloride (PVC), in which the sound velocity of the ultrasonic signal is about 1730-1800 meters/second. The material of the delay line 11 can be of silicone such as Dow Corning 3-4170 or silicone RTV such as Dow Corning 3110/3112/3120 series, in which an ultrasonic energy signal travels at a speed of about 1000 meters/second, this being slower than it will travel in the tubing material. Other suitable materials can be used depending upon the application. The delay line also can be of the same material as the tubing though which the fluid flows whose sound velocity is being measured. Here, the thickness of the material extension that forms the delay line will be greater than that of the tubing wall thickness. The delay line can be integral with the tubing, such as a protuberance on its outer wall formed during manufacture of the tubing or attached to it by a suitable process such as heat sealing or by an adhesive. As described below, in preferred embodiments of the invention the delay line is provided as a part of a measuring head in which the tubing is to be placed. The latter is preferred in applications where the tubing is to be disposable. There also can be a reflector 11 a of the ultrasonic energy signals, at the end of the delay line extension 11 that is most remote from the sensor.

The tubing first section 10A is shown as having an outer transverse length LA and an inner transverse length La. The first section, 10A can be the normal shape of the tubing. The second tubing section 10B, has smaller outer and inner transverse lengths LB and Lb produced by deformation of elastic tubing or pre-forming a rigid tubing. In each section 10A and 10B the tubing wall thickness is Lw is the same and does not change. Also, the delay line extension 11 has the same thickness Ld and is of the same material for each section 10A and 10B. The foregoing dimensions hereafter apply to all embodiments of the invention.

FIG. 2 is an embodiment of the invention for use with deformable tubing. There is a pre-molded or machined measuring head 20 which can be of any suitable material, such as plastic. The head 20 has a continuous slot 22 along its length formed by a bottom wall and two spaced opposing side walls which are generally parallel to each other and to the longitudinal axis of the tubing to be placed in the slot. The slot has a first section 22A having a known transverse length (distance across the slot between the side walls) that tapers down in a transition section 21 to a second slot section 22B having a known smaller transverse length than that of section 22A. When a piece of elastic deformable tubing 10 of greater outer diameter than that of the slot transverse length is placed in the slot 22 it will be deformed, or squeezed, to have the outer transverse lengths LA and LB (transverse length perpendicular to the two opposing slot walls) that are those of the slot of sections 22A and 22B. The transverse lengths of the slot sections 22A and 22B correspond to the transverse lengths LA and LB of the two tubing sections 10A and 10B of FIG. 1. The transverse length of the slot section 22A only has to be slightly smaller than the normal transverse lines of the deformable tubing. The slot sections transverse lengths LA and LB are known from manufacturing specifications of the measuring head 20 or from direct measuring. Since LA and LB are known and fixed, the differential value LA−LB also is known and does not change.

A respective ultrasonic transmit/receive transducer, or sensor, 30A and 30B is mounted in the head 20 in a side wall of each of the slot sections 22A and 22B. While the sensors 30A and 30B are shown on the same slot wall, one can be on the opposite walls of the slot at each of the slot sections 22A and 22B. Each sensor 30 has a face that is close to the face of the slot wall. Since the tubing in the slot is squeezed, it effectively bonds to the face of the measuring head slot wall whose material serves as a coupling medium and whose thickness is selected to be able to convey ultrasonic energy to and from each sensor and the tubing held between the slot walls. The sensors 30 can be of any suitable piezoelectric material such as PZT (lead zirconate titanate) or PVDF (PolyVinyliDene Fluoride).

A pocket 24 is formed in the measuring head 20 directly opposite each sensor 30. Each pocket 24 contains a delay line extension piece 11 behind the wall of the slot. Each delay line extension piece is of the same material and the same length so that time that the ultrasonic energy signals traveling in each piece is the same. When the tubing is placed in the slot and deformed its face effectively bonds to the slot side wall which is of a material and thickness such that the ultrasonic energy signal can be transmitted from a sensor through the slot wall into the tubing wall and the delay line extension and reflected back though these to the sensor. In applications where the delay line extension piece 11 is integral with the tubing the extension pieces would be suitably spaced along the length of the tubing so that they can be placed in openings in the side wall that correspond to the pockets 24.

In a preferred embodiment of the invention, a reflector 11 a is mounted at the bottom wall of each pocket 24. The reflector can be of any suitable material that reflects ultrasonic energy, for example a piece of metallic foil or any suitable plastic material, such as ABS, whose acoustic impedance is 3 to 4 times or more higher than that of the delay line.

The face of each sensor 30 is generally parallel to the walls of the slot, the two walls of the tubing in the two slot sections, the longitudinal axis of the tubing in the slot, and to the face of the delay line extension piece 11 opposite it. Each sensor 30 transmits an ultrasonic energy signal transverse (perpendicular) to the tubing longitudinal axis and the fluid flowing in the tubing. The ultrasonic energy signal passes through the tubing wall closest to it, the fluid flowing in the tubing, through the tubing wall remote from it and into the delay line piece 11 to be reflected back to the sensor over the same path. Thus, each sensor 30 has a respective acoustic path length APL for the signal that is transmitted by it and received after reflection from the tubing internal opposing wall. Thus, APL for 30A=2(La+Lw+Ld) APL for 30B=2(Lb+Lw+Ld) The thickness of the slot walls is not considered.

A programmable microprocessor 40 of conventional construction, preferably with an internal memory, is suitably programmed to perform the functions to be described. The microprocessor is pre-programmed with the known transverse length differential value LA−LB. The microprocessor has an output 48 which can be of any conventional type, such as a digital readout, video display, or any other suitable apparatus for displaying the results of its measurements and calculations.

The microprocessor 40 controls a transmit control circuit 42 which provides electrical signals, preferably in bursts, to each of the sensors 30A and 30B. The transmit control circuit 42 includes either a suitable source of the signals that runs continuously and whose output is gated to the sensors 30 to provide the signal bursts or a generator that the microprocessor activates for the times of the bursts. The microprocessor 40 also operates a multiplexer 50 that controls transmission and reception of the signals by the sensors 30A and 30B. The electrical signals provided to each sensor 30 by the transmit control circuit 42 are converted into electro-mechanical (ultrasonic) energy signals that are transmitted by the sensor. The ultrasonic signals pass through the tubing wall closest to the sensor, the fluid flowing in the tubing, the tubing wall remote from the sensor, into the delay line piece to be reflected from the end of the delay line piece or the reflector back over the same path to the sensor. This is sometimes called the pulse echo technique. The sensor 30 then converts the received reflected electro-mechanical energy back to an electrical signal.

Microprocessor 40 also operates to control the transmission of the signals by each sensor and the reception of the reflected signals. That is, there is a pause between the transmission of each burst of signals by a sensor to allow for reception of the reflected energy and the calculation of the round-trip transit time before the next signal burst is transmitted. A high speed amplifier 44 receives the signal from each sensor 30A and 30B of the energy reflected from the internal wall of each tubing section 22A and 22B. A feedback control circuit 52 is provided to normalize the amplitude of the received signals to a substantially fixed value and these signals are applied to a high speed analog/digital (A/D) converter 46 to be converted to digital form. The digital signals are applied to the microprocessor 40 for use in various computational functions. In a preferred embodiment of the invention, the microprocessor is programmed to open a gate (not shown) in the electronic circuit at the approximate time to provide a window when the reflected signal to be used for the round-trip transit time calculation is to be received. This further aids in the discrimination against the reverberations of the sensor during transmission.

The time of transmission of the energy by each sensor 30 is known at the microprocessor 40 since it controls this time. The microprocessor also knows the time of reception of the reflected signals as supplied by the A/D converter 46. Therefore, the microprocessor can calculate the round trip transit time of the signals transmitted from each sensor 30 and received back to it after reflection from the tubing opposing inner wall. Alternate methods of calculating the round-trip transit time can be used such as starting a clock running at the time of the signal transmission and stopping the clock at the time of the reflected signal reception.

The circuit preferably operates so that the two round-trip transit times of the signals in the tubing sections 22A and 22B are measured sequentially or at substantially the same time. In a preferred embodiment of the invention, the two transit times are measured as close to simultaneously as possible so that any change in the temperature of the fluid flowing in the tubing 10 between the two slot sections 22A and 22B will not adversely affect the accuracy of the measurements and the final calculation of the sound velocity. If desired, the measuring head can be provided with a non-invasive sensor for measuring the temperature, such as described in U.S. Pat. No. 7,661,294 granted to the inventor of this invention, to improve the accuracy of the measurements.

The calculation of the sound velocity is explained as follows.

At each point of the slot where there is a sensor 30 the tubing outer transverse lengths LA and LB including the delay line extension pieces can be written as LA=2Lw+La−Ld  (1) and LB=2Lw+Lb−Ld  (2) where:

LA and LB are the outer transverse lengths of the two tubing sections.

Lw=wall thickness of a given tubing. This is the same for both tubing sections and does not change at the location of the tubing deformation from the tubing normal overall shape.

Ld=the length of the delay line extension piece in each pocket. These are the same for both of the slot sections with or without a reflector.

La=tubing inner transverse length at slot section 22A at which sensor 30A is located.

Lb=tubing inner transverse length at sensor 30B location in slot section 22B.

From equations (1) and (2): LA−LB=La−Lb, hereafter called LAB  (3) where

LAB=fixed differential of the tubing outer transverse lengths at the locations of sensors 30A and 30B. LAB is known from the cross-sectional lengths of the slot in each of the sections 22A and 22B which sets each of LA and LB. The value of LAB is programmed into the microprocessor.

Using the pulse echo technique with a single sensor 30 at a point of each slot section 22A and 22B, the respective round trip travel time ta and tb of the energy at each sensor location of the slot sections 22A and 22B is determined as follows:

$\begin{matrix} {{{ta} = {\frac{2{tw}}{Vw} + \frac{2{La}}{V} + \frac{2{Ld}}{Vd}}}{{tb} = {\frac{2{tw}}{Vw} + \frac{2{Lb}}{V} + \frac{2{Ld}}{Vd}}}} & (4) \end{matrix}$ where,

Vw=the velocity of the ultrasonic energy signal in the tubing walls.

V=the velocity of the ultrasonic energy signal in the liquid flowing in the tubing.

Vd=The velocity of the ultrasonic energy signal in the delay line extension piece. This can be different from Vw.

Therefore:

$\begin{matrix} {{{ta} - {tb}} = \frac{2\left( {{La} - {Lb}} \right)}{V}} & (6) \end{matrix}$ As seen from equation (6) the tubing wall thickness Lw cancels, meaning that the measurement is independent of this quantity. In a similar manner, if the thickness of the slot wall at the pocket 24 containing the delay line is considered, it also would cancel out meaning that the measurement is independent of each slot wall.

Since from equation (3), La−Lb=LA−LB=LAB, therefore:

$\begin{matrix} {V = \frac{2{LAB}}{{ta} - {tb}}} & (7) \end{matrix}$ where ta−tb is the differential of the two round trip measurements. Let: ta−tb=tab so that

$\begin{matrix} {V = \frac{2{LAB}}{tab}} & (8) \end{matrix}$

Thus, by knowing the fixed differential LAB of the transverse lengths at the points of each of the sensors 30A and 30B, as set by the transverse lengths of the measuring head slot sections 22A and 22B, and measuring the two round trip times ta and tb, from which the differential elapsed time tab is calculated, the sound velocity V of the flowing fluid is calculated by the microprocessor using equation (8).

It is noted that the sound velocity of both the tubing wall Lw and that of the delay line extension piece Ld is different from that of the flowing liquid. However, as shown above in equation (8), the sound velocity measurement is independent of both the tubing wall thickness Lw and the length of the delay line extension piece Ld. As also can be seen from equation (8), the accuracy of the measurement can be increased by increasing the differential LAB of the transverse lengths of the two sections because tab remains the same.

Typical parameters for the instrument of the invention, by way of example, are:

a. material of tubing (deformable or rigid)—PVC, Teflon, any plastic material, metal, glass and capillary type tubings.

b. outside diameter of tubing before squeeze—⅛″ minimum to 1″ maximum.

c. wall thickness of tubing 0.01″ to 0.1″maximum

d. tubing inner and outer transverse lengths after squeeze—, approximately 20% to 30% less than before, the squeeze. The tubing wall thickness Lw is not changed by the squeeze.

e. distance between the two sensors 30A and 30B—minimum 0.5″, maximum 2.0″.

f. transverse length LA and LB across the slot at the two sections 22A and 22B—different for each tubing and accuracy desired.

g. length of slot sections 22A and 22B—0.25″ to 1.00″ or more, and being independent of the transition between the two sections.

h. operating frequency—2 MHZ minimum-20 MHZ maximum, depends on resolution of system that is desired.

I. duration of pulse bursts of the ultrasonic energy. Minimum 100 nano seconds, Maximum 1 microsecond.

j. time between the bursts—10 microseconds minimum to 5 milliseconds maximum.

Other frequencies, burst durations and burst timing as well as other physical dimensions can be used depending on the material and size of the tubing, the type of fluid and the accuracy of the result needed.

FIG. 3 shows a further embodiment of the invention in which both of the sensors are positioned at a single location along the tubing length. The same reference numerals are used for the same components of the embodiment of FIG. 2. Here, there is a measuring head 80 that has a slot 82 in which the tubing is placed. The slot 82 has a transverse dimension LA across its width so that when the tubing is placed in the slot it will have the same outer transverse length dimension LA that corresponds to the first tubing section 10A of FIGS. 1 and 2. There is a cover 83 at the top of the slot 82 whose inner surface together with the bottom wall of the slot sets the transverse length dimension LB. The cover 83 can be hinged to the measuring head, have a snap fit, slide over the slot location, or any other suitable type of fastening configuration. The tubing 10 in the slot 82 has an original dimension such that when deformed in the slot it will engage the inner wall of the cover 83. The tubing therefore will assume a second transverse length LB that is orthogonal to the first length LA and corresponds to the second tubing section 10B of FIGS. 1 and 2. The tubing will have its normal circular shape in locations outside of the slot 82. Therefore, the transverse length differential LA−LB (LAB) is known and fixed.

The two transmit/receive sensors 30A and 30B are mounted in the measuring head 80 at an angle to each other at two different points at one location along the slot length to address respective tubing first and second transverse lengths LA and LB. As shown in FIG. 3, sensor 30A is at a side wall of the slot and sensor 30B at the bottom wall, making the sensors orthogonal to each other. A delay line extension piece 11 and a reflector 11 a are located in a pocket 24 in the measuring head wall opposite the sensor 30A. This extends the ultrasonic energy signal path in the direction of the tubing transverse length LA. Also, a delay line extension piece 11 and reflector 11 a are located on the inside of the cover 83 to extend the ultrasonic energy signal path in the direction of the tubing transverse length LB. The faces of the two sensors 30A and 30B oppose the delay line pieces 11 and are parallel to the axis of the fluid flowing in the tubing and to the tubing outer wall and transmit energy generally transverse to each. The travel path for the ultrasonic energy signal is as described with respect to FIG. 2, that is, one wall of the tubing, the liquid flowing in the tubing, another wall of the tubing, into the delay line extension piece from which it is reflected back to the sensor over the same path.

The circuit of the embodiment of FIG. 3 operates similarly to that of FIG. 2 in that the two sensors 30A and 30B are supplied with signals from the transmit control circuit 42. The round-trip transit time of the signals transmitted by each sensor and received after reflection from the end of the delay line is measured in the manner described above, with respect to equations (1)-(4). The sound velocity of the signal is also calculated in the same manner as described above with respect to equations (5)-(8).

FIG. 4 shows another embodiment of the invention that is useful with semi-rigid or rigid tubing, that is, tubing that cannot be readily deformed such as by placing it in a slot. Here there is a tubing 96 of a rigid or semi-rigid material such as hard or soft PVC that is configured with two sections 96A and 96B of different outer and inner diameters and the same wall thickness in each section. There can be a transition section between the two sections if needed or desired, such as shown in FIG. 2. The two tubing sections can be molded in the desired shape or be joined by any suitable coupling or transition member (not shown) that couples the two tubing sections of different diameters together. If the tubing is of metal, the ends of tubing sections of different diameter can be welded or soldered together. The tubing sections 96A and 96B can be of any shape with circular shape being preferred. The outer diameters of the tubing sections 96A and 96B correspond to the transverse lengths LA and LB of tubing 10 of FIGS. 1-3 and the inner diameters correspond to the transverse lengths La and Lb of FIGS. 1-3.

A measuring head 90 is used that has a slot 92 with sections 92A and 92B each of a transverse width that corresponds to the respective outer diameters of the two tubing sections 96A and 96B. The transverse and elongated lengths of the slot sections are selected as fits the application of needed accuracy and material and dimensions of the tubing sections. There is a sensor 30A and 30B in the head 90 at the wall of each of the slot sections 92A and 92B. In this embodiment of the invention, the rigid tubing 96 is placed in slot 92 so that the respective sensors 30A and 30B are opposite and contact the corresponding wall of the tubing sections 96A and 96B. There is no deformation of the tubing 96 as it is placed in the slot 92. If desired, a coupling material such as petroleum jelly can be used between the sensors and the tubing outer wall. Also if desired, the two sensors can be mounted directly to the wall of the tubing thereby eliminating the need for the head 90.

As in the case of embodiment of FIG. 2, there is a pocket 24 in the wall of the head and 90 opposite each sensor 30 and a delay line extension piece 11 and reflector 11 a are provided in each pocket. The ultrasonic energy signal transmitted by each sensor 30 travels the same path as described above from the sensor, through the fluid and the tubing walls to the end of the delay line extension piece to be reflected back to the sensor over the same path.

The operation of the apparatus of FIG. 4 is the same as that previously described in that the round-trip transit time of the signals from each of the sensors 30A and 30B in the first and second acoustic paths of the tubing sections 92A and 92B will each be measured by the microprocessor 40 using equations (2)-(4). From these measurements and the known differential LAB of the tubing sections transverse lengths, which are pre-programmed into the microprocessor 40, the sound velocity of the flowing fluid will be calculated as described above using the equations (5)-(8).

The invention has a number of advantages. The microprocessor 40 can be programmed to calculate and provide any property or characteristic of the fluid that can be determined using the sound velocity information that has been calculated. Thus, the invention can provide on-line real time measurement of liquid properties and characteristics using sound velocity information. In addition, the use of a delay line extension piece makes it easier to identify the reflected signal in the pulse echo technique to be used for measuring the round-trip transit time in applications where the internal diameter of the tubing passageway through which the fluid flows is relatively small or is small in comparison to the thickness of the tubing wall.

The disposable elastic tubing of various types of existing equipment can be utilized without modification in utilizing the invention. Also, there is no need to design special fixtures or cups of specific acoustic length since the calculation of the sound velocity is independent of fluid flow rate change, and tubing wall thickness. In many situations it is also relatively independent of temperature change. The invention is useful in industrial applications such as where corrosive liquids, e.g. H₂SO₄, HNO₃ can be monitored continuously.

Specific features of the invention are shown in one or more of the drawings for convenience only, as each feature may be combined with other features in accordance with the invention. Alternative embodiments will be recognized by those skilled in the art and are intended to be included within the scope of the claims. Accordingly, the above description should be construed as illustrating and not limiting the scope of the invention. All such obvious changes and modifications are within the patented scope of the appended claims. 

I claim:
 1. Apparatus for noninvasive measurement of the sound velocity of a fluid flowing in a tubing, comprising: a measuring head having an open slot with a flat planar bottom wall and two flat planar opposing side walls in which the tubing is placed, the bottom and side walls are orthogonal to each other and are arranged such that both ends of the bottom wall are contacted by one end of each of the two side walls, which walls contact the tubing, said slot having first and second points of different transverse length being at different locations of the slot longitudinal length, each slot transverse length at said first and second points forming a respective acoustic path of a different length; a source of ultrasonic energy signals; a respective first and second transmit/receive sensor mounted in said measuring head adjacent said slot first and second points of different transverse length; a delay line of the same material and length opposing each said sensor on the opposite side of the tube, each said sensor for transmitting signals from said energy source along a respective path through the walls of the tubing and the fluid flowing therein into the respective opposing delay line element on the opposition side of the tube and receiving the signals reflected from the delay line element back to a said sensor; and a circuit for measuring for each said first and second sensor the round-trip transit time of the signals from time of transmission to the time of reception after reflection from the delay line element, and for calculating from the round-trip transit times measured for the signals of the first and second sensors the sound velocity of the fluid flowing in the tubing.
 2. The apparatus as claimed in claim 1 wherein said circuit calculates the sound velocity also based on the differential of the transverse lengths at said first and second points of said slot.
 3. The apparatus as claimed in claim 2 wherein the different transverse lengths are determined by the lengths between the opposing walls of the slot and are known by said circuit before the calculation of sound velocity takes place.
 4. The apparatus as claimed in claim 2 wherein said slot is to hold an elastic tubing and has dimensions such as to deform the tubing to produce the different transverse lengths forming the different paths for said first and second sensors.
 5. The apparatus as claimed in claim 4 wherein: said slot is elongated and has first and second sections of different transverse length across the slot of the respective first and second section in which the tubing is to be placed to have a respective different transverse length across a tubing in each slot section; and wherein said first and second sensors are mounted in said head at a respective corresponding point in a wall of a said slot first and second section.
 6. The apparatus as claimed in claim 4 wherein the walls of said slot are generally parallel and are to be generally parallel to the longitudinal axis of the tubing.
 7. The apparatus as claimed in claim 2 wherein said slot is elongated and has first and second sections of different transverse length across the respective section and a rigid tubing having matching first and second sections of different transverse length is placed in the slot; and wherein said first and second sensors are mounted in said head at a respective point of said first and second slot section.
 8. The apparatus as claimed in claim 2 wherein said circuit operates to calculate the sound velocity V using the formula $V = \frac{2{LAB}}{tab}$ where: LAB=the differential of the transverse lengths at the two points, and tab=the differential of the two round trip time measurements.
 9. The apparatus as claimed in claim 1 wherein said circuit comprises a microprocessor for controlling the times of transmission of the signals, measuring the round trip transit times and calculating the sound velocity.
 10. The apparatus as claimed in claim 9 wherein said microprocessor operates to calculate the sound velocity V using the formula $V = \frac{2{LAB}}{tab}$ where: LAB=the differential of the transverse lengths at the two points, and tab=the differential of the two round trip time measurements.
 11. The apparatus as claimed in claim 1 wherein each said delay line is of a material having a different velocity of travel of the ultrasonic energy signal than the velocity of travel of the ultrasonic energy signal through the tubing and the fluid flowing therein.
 12. The apparatus as claimed in claim 1 wherein each said delay line is of an elastomeric material.
 13. The apparatus as claimed in claim 1 further comprising: a respective pocket at one wall of said slot in said measuring head at each of said first and second points in which said delay line is located; and wherein said sensor is located at the other wall of said slot first and second points to transmit the energy through the tubing into said delay line.
 14. The apparatus as claimed in claim 1 further comprising a reflector at the end of each delay line from which the ultrasonic energy signals are reflected.
 15. Apparatus for noninvasive measurement of the sound velocity of a fluid flowing in a tubing, comprising: a measuring head having an open slot with a flat planar bottom wall and two flat planar opposing side walls in which the tubing is placed, the bottom and side walls are orthogonal to each other and are arranged such that both ends of the bottom wall are contacted by one end of each of the two side walls, which walls contact the tubing; a cover with a portion that extends into the open end of the slot and contacts the tubing; said slot having first and second points of different transverse length, said first point forming a first acoustic path between the side walls of the slot and said second point forming a second acoustic path between the cover and bottom of the slot, said first and second acoustic paths being of different lengths; a source of ultrasonic energy signals; a respective first and second transmit/receive sensor mounted in said measuring head adjacent said first and second acoustic paths of different transverse length; a delay line of the same material and length opposing each said sensor on the opposite side of the tube, each said sensor for transmitting signals from said energy source along a respective path through the walls of the tubing and the fluid flowing therein into the respective opposing delay line element on the opposition side of the tube and receiving the signals reflected from the delay line element back to a said sensor; and a circuit for measuring for each said first and second sensor the round-trip transit time of the signals from time of transmission to the time of reception after reflection from the delay line element, and for calculating from the round-trip transit times measured for the signals of the first and second sensors the sound velocity of the fluid flowing in the tubing wherein said slot provides the first and second points at one location along the length of the tubing, and said first and second sensors are mounted in said measuring head at different walls of said slot or the cover that are generally orthogonal to each other.
 16. The apparatus as claimed in claim 15 wherein the tube naturally has a round shape, but is squeezed by the opposing side walls of the slot into an oval shape, one sensor is located in one side wall of the slot and the delay line is located in a pocket in the opposite side wall, the second sensor is located in the bottom wall of the slot; and wherein an inner wall of the cover is curved so as to engage and contact the oval shape of the tube opposite the bottom wall, said delay line for the second acoustic path being located in a pocket behind the curved wall in the cover.
 17. The apparatus as claimed in claim 16 wherein each delay line includes a reflector at its end.
 18. Apparatus for measuring the round-trip travel time of an ultrasonic energy signal in a tubing through which a fluid is flowing, comprising: a delay line providing a predetermined delay located adjacent to and on only one side of the tubing; a sensor on the opposite side of the tubing from the delay line for transmitting and an ultrasonic energy signal through the walls of the tubing and the fluid flowing there through, into said delay line to be reflected from said delay line back through the tubing and the fluid to said sensor; and an electronic circuit for measuring the round-trip transit time of the ultrasonic signal from transmission from said sensor and reflection back to said sensor.
 19. The measuring apparatus as claimed in claim 18 wherein said delay line is of a material having a different velocity of travel of the ultrasonic energy signal than the velocity of travel of the ultrasonic energy signal through the tubing and the fluid flowing therein.
 20. The measuring apparatus as claimed in claim 18 further comprising a reflector for said ultrasonic energy signal at the end of said delay line.
 21. The measuring apparatus as claimed in claim 18 further comprising: a measuring head having an open slot formed by a flat planar bottom wall and two flat planar opposing side walls within which said tubing is to be placed, the bottom and side walls are orthogonal to each other and are arranged such that both ends of the bottom wall are contacted by one end of each of the two side walls, which walls contact the tubing; a pocket at one wall of said slot in said measuring head within which said delay line is located; and wherein said sensor is located at the other wall of said slot to transmit the energy through the tubing into said delay line to be reflected back to said sensor.
 22. The measuring apparatus as claimed in claim 21 further comprising a reflector for said ultrasonic energy signal at the end of said delay line. 